Table A.1
Impact of free parameters in our modelling
| Ex situ in 0.95 boundary % | In situ in 0.05 boundary % | Nexsitu | Nmixing zone | Ninsitu | |
|---|---|---|---|---|---|
| Fiducial model | 81.21 | 76.4 | 67 | 38 | 55 |
| Fixed disk potential | 81.28 | 74.97 | 67 | 40 | 53 |
| In situ tagged at z = 3 | 83.13 | 23.45 | 78 | 68 | 14 |
M⊙ |
80.27 | 41 | 65 | 30 | 65 |
M⊙ |
81.38 | 96.5 | 68 | 49 | 43 |
| Mass loss | |||||
| (γ = 0.7 & t0,⊙ = 10.7 Myr) | 80.83 | 54.17 | 66 | 32 | 62 |
Notes: From left to right, the columns report, for each configuration: the percentage of simulated GCs classified as ex situ and in situ using the 0.95 and 0.05 decision boundaries, respectively, as well as the number of GCs identified as ex situ, in the mixing zone, and in situ. Our fiducial model assumes 106 M⊙ GCs tagged at z = 2 for in situ clusters and at z = 3 for ex situ ones, evolved in MW-like potentials without a disk component, with mass loss parametrized by γ = 0.62 and t0,⊙ = 21.3 Myr. The fixed disk is modelled using a Miyamoto & Nagai (1975) potential with a mass of 6.8 × 1010 M⊙, a scale length a = 3 kpc, and a scale height b = 280 pc, consistent with the MWPotential2014 used in Bovy (2015).
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![$\[M_{\mathrm{GC}}^{\text {ini}}=5 \times 10^{5}\]$](/articles/aa/full_html/2025/12/aa55964-25/aa55964-25-eq16.png)
![$\[M_{\text {GC}}^{\text {ini}}=5 \times 10^{6}\]$](/articles/aa/full_html/2025/12/aa55964-25/aa55964-25-eq17.png)